Book contents
- Frontmatter
- Contents
- Preface
- Glossary
- Nomenclature
- Part 1 Design of Engines for a New 600-seat Aircraft
- Part 2 Engine Component Characteristics and Engine Matching
- Part 3 Design of Engines for a New Fighter Aircraft
- 13 A New Fighter Aircraft
- 14 Lift, Drag and the Effects of Manoeuvring
- 15 Engines for Combat Aircraft
- 16 Design Point for a Combat Engine
- 17 Combat Engines Off-design
- 18 Turbomachinery for Combat Engines
- Part 4 Return to the Civil Transport Engine
- Appendix: Noise and its Regulation
- Bibliography
- References
- Index
- Design sheets for New Large Civil Aircraft and New Fighter Aircraft
14 - Lift, Drag and the Effects of Manoeuvring
from Part 3 - Design of Engines for a New Fighter Aircraft
- Frontmatter
- Contents
- Preface
- Glossary
- Nomenclature
- Part 1 Design of Engines for a New 600-seat Aircraft
- Part 2 Engine Component Characteristics and Engine Matching
- Part 3 Design of Engines for a New Fighter Aircraft
- 13 A New Fighter Aircraft
- 14 Lift, Drag and the Effects of Manoeuvring
- 15 Engines for Combat Aircraft
- 16 Design Point for a Combat Engine
- 17 Combat Engines Off-design
- 18 Turbomachinery for Combat Engines
- Part 4 Return to the Civil Transport Engine
- Appendix: Noise and its Regulation
- Bibliography
- References
- Index
- Design sheets for New Large Civil Aircraft and New Fighter Aircraft
Summary
INTRODUCTION
A fighter aircraft is required to be agile, which requires it to turn sharply, to accelerate rapidly and usually to travel fast. It is no surprise that accelerating rapidly or travelling fast require large amounts of thrust from the engine. What may be more of a surprise is that rapid changes in direction require high levels of engine thrust. The reason is that the drag of the aircraft rises approximately with the square of the lift coefficient and making rapid turns demands high lift from the wings. An aircraft normally banks in order to turn so that the resultant of the gravitation acceleration and the centripetal acceleration is normal to the plane of the wings, Fig. 14.1, and the force they produce is exactly balanced by the wing lift. It is normal to express the increase in acceleration in terms of the load factor, denoted by n: a load factor of unity corresponds to an acceleration g perpendicular to the wing, when the lift is the normal weight of the aircraft, whereas a load factor of 5 corresponds to an acceleration of 5g and the lift is five times the weight. For a modern fighter aircraft structures are designed to withstand the approximate limit on acceleration set by the human pilot and load factors can be as high as 9.
For the civil airliner the turns are normally so gentle that the lift on the wings is little more than the weight of the aircraft, and the size of the engine is normally fixed by requirements at the top of the climb.
- Type
- Chapter
- Information
- Jet PropulsionA Simple Guide to the Aerodynamic and Thermodynamic Design and Performance of Jet Engines, pp. 189 - 200Publisher: Cambridge University PressPrint publication year: 2003